Finite-size scaling analysis of localization transitions in the disordered two-dimensional Bose-Hubbard model within the fluctuation operator expansion method

TL;DR

This paper investigates the localization transition in the disordered two-dimensional Bose-Hubbard model, analyzing the mobility edge and finite-size effects using the fluctuation operator expansion method.

Contribution

It introduces a finite-size scaling analysis of the localization transition and mobility edge in the disordered 2D Bose-Hubbard model using the fluctuation operator expansion.

Findings

Level spacing statistics indicate a many-body mobility edge.

Finite-size scaling reveals corrections to the superfluid-Bose-glass transition.

Spectral properties differ above and below the mobility edge.

Abstract

The disordered Bose-Hubbard model in two dimensions at non-integer filling admits a superfluid to Bose-glass transition at weak disorder. Less understood are the properties of this system at strong disorder and energy densities corresponding to excited states. In this work we study the Bose-glass transition of the ground state and the related finite energy localization transition, the mobility edge of the quasiparticle spectrum, a critical energy separating extended from localized quasiparticle excitations. To study these the fluctuation operator expansion is used. The level spacing statistics of the quasiparticle excitations, the fractal dimension and decay of the corresponding wave functions are consistent with a many-body mobility edge. The finite-size scaling of the lowest gaps yields a correction to the mean-field prediction of the superfluid to Bose-glass transition. In its vicinity we discuss spectral properties of the ground state in terms of the dynamic structure factor and the spectral function which also shows distinct behavior above and below the mobility edge.